Dynamic stability research on rectangular thin plate based on the quadratic eigenvalue method
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Dynamic stability research on rectangular thin plate based on the quadratic eigenvalue method
Acta Scientiarum Naturalium Universitatis SunYatseniVol. 55, Issue 3, Pages: 68-76(2016)
作者机构:
广州大学-淡江大学工程结构灾害与控制联合研究中心,广东,广州,510006
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Published:2016,
Published Online:25 May 2016,
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ZHONG Zilin, LIU Airong, LU Hanwen, et al. Dynamic stability research on rectangular thin plate based on the quadratic eigenvalue method. [J]. Acta Scientiarum Naturalium Universitatis SunYatseni 55(3):68-76(2016)
DOI:
ZHONG Zilin, LIU Airong, LU Hanwen, et al. Dynamic stability research on rectangular thin plate based on the quadratic eigenvalue method. [J]. Acta Scientiarum Naturalium Universitatis SunYatseni 55(3):68-76(2016)DOI:
Dynamic stability research on rectangular thin plate based on the quadratic eigenvalue method
Based on the Von-Karman large deflection theory of thin plates
the second-order ordinary differential Mathieu-hill Parametric vibration equation was established for of simply supported rectangular thin plate under in-plane periodic loading using the Galerkin method. The quadratic eigenvalue method was adopted to obtain the main and secondary instability domains of the rectangular thin plate with the periodic solutions of 2T and T
then the accuracy of the method was verified by finite element method
meanwhile
the influence of nonlinear elasticity on stationary amplitude caused by the main Parametric resonance was qualitatively analyzed. The analytic results showed that strong transverse parametric resonance will occur when the frequency of excitation force is about twice as large as the natural vibration frequency of the thin plate. The quadratic eigenvalue method can be used to calculate accurately those parameters
such as the frequency and the excitation coefficient of the dynamic instability region of the rectangular thin plate. As the increasing of the amplitude
the infinite increase of vibration amplitude was controlled owing to the nonlinear factor which tows system to the direction of large vibration frequency. Furthermore
the nonlinear factor can bring the system into a complex vibration state in which the vibration amplitude increased stably or rapidly.